The intuition for solving the tension between the observed Higgs mass and perturbativity
is obvious in the context of SUSY.
The main observation is that Yukawa couplings in superpotential receive only wave-function induced renormalizations due to the protection of SUSY,
in contrast to non-supersymmetric case The phenomenon of Yukawa coupling being asymptotically free has been exposed in \(\lambda \phi ^{4}\)  scalar field theory with dimension lower than four by Wilson and Fisher [1]},
and in well-known nonlinear sigma model [2]} together with an attempt to obtain a version of four-dimensional supersymmetry [3]}.
Similar phenomenon was also addressed by authors of [4]} in four-dimensional scalar field theory with nonpolynomial potentials..
By following the fact that the beta functions of Yukawa couplings are related to the anomalous dimensions of chiral fields [5]},
and the anomalous dimensions are proportional to quadratic Yukawa couplings with positive coefficients,
the sign of contribution to \(\beta \)  function due to Yukawa interactions is thus always positive.
A way to alleviate this is introducing hidden super-confining gauge dynamics [6]}, [7]},
from which Yukawa couplings are asymptotically free,
and \(S\)  is a composite other than fundamental state,
with large \(\lambda \)  at low energy as a result of this asymptotical freedom.
In this context the Higgs doublets can be either fundamental [6]} or composite states [7]}.
